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Measurements of both the inclusive and differential production cross sections of a top-quark-antiquark pair in association with a $Z$ boson ($t\bar{t}Z$) are presented. The measurements are performed by targeting final states with three or four isolated leptons (electrons or muons) and are based on $\sqrt{s} = 13$ TeV proton-proton collision data with an integrated luminosity of 139 fb$^{-1}$, recorded from 2015 to 2018 with the ATLAS detector at the CERN Large Hadron Collider. The inclusive cross section is measured to be $\sigma_{t\bar{t}Z} = 0.99 \pm 0.05$ (stat.) $\pm 0.08$ (syst.) pb, in agreement with the most precise theoretical predictions. The differential measurements are presented as a function of a number of kinematic variables which probe the kinematics of the $t\bar{t}Z$ system. Both absolute and normalised differential cross-section measurements are performed at particle and parton levels for specific fiducial volumes and are compared with theoretical predictions at different levels of precision, based on a $\chi^{2}/$ndf and $p$-value computation. Overall, good agreement is observed between the unfolded data and the predictions.
The measured $t\bar{t}\text{Z}$ cross-section value and its uncertainty based on the fit results from the combined trilepton and tetralepton channels. The value corresponds to the phase-space region where the difermion mass from the Z boson decay lies in the range $70 < m_{f\bar{f}} < 110$ GeV.
List of relative uncertainties of the measured inclusive $t\bar{t}\text{Z}$ cross section from the combined fit. The uncertainties are symmetrised for presentation and grouped into the categories described in the text. The quadratic sum of the individual uncertainties is not equal to the total uncertainty due to correlations introduced by the fit.
The definitions of the trilepton signal regions: for the inclusive measurement, a combination of the regions with pseudo-continuous $b$-tagging 3$\ell$-Z-1$b$4$j$-PCBT and 3$\ell$-Z-2$b$3$j$-PCBT is used, whereas for the differential measurement, only the region 3$\ell$-Z-2$b$3$j$, with a fixed $b$-tagging WP is employed.
The definitions of the four tetralepton signal regions. The regions are defined to target different $b$-jet multiplicities and flavour combinations of the non-Z leptons.
The absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}$ of the $Z$ boson in the 3$\ell$+4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}$ of the $Z$ boson in the 3$\ell$+4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}$ of the $Z$ boson in the 3$\ell$+4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}$ of the $Z$ boson in the 3$\ell$+4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the absolute value of rapidity of the $Z$ boson in the 3$\ell$+4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the number of jets in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the number of jets in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{l \textrm{non-}Z}$ in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (Z, t_{\textrm{lep}})|/\pi$ in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta y (Z, t_{\textrm{lep}})|$ in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (l_{t}^{+}, l_{\bar{t}}^{-})|/\pi$ in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (t\bar{t}, Z)|/\pi$ in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{t\bar{t}}$ in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{l \textrm{non-}Z}$ in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (Z, t_{\textrm{lep}})|/\pi$ in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta y (Z, t_{\textrm{lep}})|$ in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (l_{t}^{+}, l_{\bar{t}}^{-})|/\pi$ in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (t\bar{t}, Z)|/\pi$ in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{t\bar{t}}$ in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the absolute value of rapidity of the $Z$ boson in the 3$\ell$+4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{l \textrm{non-}Z}$ in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (Z, t_{\textrm{lep}})|/\pi$ in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta y (Z, t_{\textrm{lep}})|$ in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (l_{t}^{+}, l_{\bar{t}}^{-})|/\pi$ in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (t\bar{t}, Z)|/\pi$ in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{t\bar{t}}$ in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the absolute value of rapidity of the $Z$ boson in the 3$\ell$+4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{l \textrm{non-}Z}$ in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (Z, t_{\textrm{lep}})|/\pi$ in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta y (Z, t_{\textrm{lep}})|$ in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (l_{t}^{+}, l_{\bar{t}}^{-})|/\pi$ in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (t\bar{t}, Z)|/\pi$ in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{t\bar{t}}$ in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the absolute value of rapidity of the $Z$ boson in the 3$\ell$+4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the number of jets in the 3$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the number of jets in the 4$\ell$ channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The total correlation matrix of the absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}$ of the $Z$ boson in the 3$\ell$+4$\ell$ channel.
The total correlation matrix of the absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the absolute value of rapidity of the $Z$ boson in the 3$\ell$+4$\ell$ channel.
The total correlation matrix of the absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{l \textrm{non-}Z}$ in the 3$\ell$ channel.
The total correlation matrix of the absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (Z, t_{\textrm{lep}})|/\pi$ in the 3$\ell$ channel.
The total correlation matrix of the absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta y (Z, t_{\textrm{lep}})|/\pi$ in the 3$\ell$ channel.
The total correlation matrix of the absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (l_{t}^{+}, l_{\bar{t}}^{-})|/\pi$ in the 4$\ell$ channel.
The total correlation matrix of the absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (t\bar{t}, Z)|/\pi$ in the 4$\ell$ channel.
The total correlation matrix of the absolute parton-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{t\bar{t}}$ in the 4$\ell$ channel.
The total correlation matrix of the normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}$ of the $Z$ boson in the 3$\ell$+4$\ell$ channel.
The total correlation matrix of the normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the absolute value of rapidity of the $Z$ boson in the 3$\ell$+4$\ell$ channel.
The total correlation matrix of the normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{l \textrm{non-}Z}$ in the 3$\ell$ channel.
The total correlation matrix of the normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (Z, t_{\textrm{lep}})|/\pi$ in the 3$\ell$ channel.
The total correlation matrix of the normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta y (Z, t_{\textrm{lep}})|/\pi$ in the 3$\ell$ channel.
The total correlation matrix of the normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (l_{t}^{+}, l_{\bar{t}}^{-})|/\pi$ in the 4$\ell$ channel.
The total correlation matrix of the normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (t\bar{t}, Z)|/\pi$ in the 4$\ell$ channel.
The total correlation matrix of the normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{t\bar{t}}$ in the 4$\ell$ channel.
The total correlation matrix of the absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}$ of the $Z$ boson in the 3$\ell$+4$\ell$ channel.
The total correlation matrix of the absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the absolute value of rapidity of the $Z$ boson in the 3$\ell$+4$\ell$ channel.
The total correlation matrix of the absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{l \textrm{non-}Z}$ in the 3$\ell$ channel.
The total correlation matrix of the absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (Z, t_{\textrm{lep}})|/\pi$ in the 3$\ell$ channel.
The total correlation matrix of the absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta y (Z, t_{\textrm{lep}})|/\pi$ in the 3$\ell$ channel.
The total correlation matrix of the absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the number of jets in the 3$\ell$ channel.
The total correlation matrix of the absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (l_{t}^{+}, l_{\bar{t}}^{-})|/\pi$ in the 4$\ell$ channel.
The total correlation matrix of the absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (t\bar{t}, Z)|/\pi$ in the 4$\ell$ channel.
The total correlation matrix of the absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{t\bar{t}}$ in the 4$\ell$ channel.
The total correlation matrix of the absolute particle-level differential cross-section measured in the fiducial phase-space as a function of the number of jets in the 4$\ell$ channel.
The total correlation matrix of the normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}$ of the $Z$ boson in the 3$\ell$+4$\ell$ channel.
The total correlation matrix of the normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the absolute value of rapidity of the $Z$ boson in the 3$\ell$+4$\ell$ channel.
The total correlation matrix of the normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{l \textrm{non-}Z}$ in the 3$\ell$ channel.
The total correlation matrix of the normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (Z, t_{\textrm{lep}})|/\pi$ in the 3$\ell$ channel.
The total correlation matrix of the normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta y (Z, t_{\textrm{lep}})|/\pi$ in the 3$\ell$ channel.
The total correlation matrix of the normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the number of jets in the 3$\ell$ channel.
The total correlation matrix of the normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (l_{t}^{+}, l_{\bar{t}}^{-})|/\pi$ in the 4$\ell$ channel.
The total correlation matrix of the normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (t\bar{t}, Z)|/\pi$ in the 4$\ell$ channel.
The total correlation matrix of the normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the $p_{\textrm{T}}^{t\bar{t}}$ in the 4$\ell$ channel.
The total correlation matrix of the normalised particle-level differential cross-section measured in the fiducial phase-space as a function of the number of jets in the 4$\ell$ channel.
A measurement of event-shape variables in proton$-$proton collisions at large momentum transfer is presented using data collected at $\sqrt{s} = 13$ TeV with the ATLAS detector at the Large Hadron Collider. Six event-shape variables calculated using hadronic jets are studied in inclusive multijet events using data corresponding to an integrated luminosity of 139 fb$^{-1}$. Measurements are performed in bins of jet multiplicity and in different ranges of the scalar sum of the transverse momenta of the two leading jets, reaching scales beyond 2 TeV. These measurements are compared with predictions from Monte Carlo event generators containing leading-order or next-to-leading order matrix elements matched to parton showers simulated to leading-logarithm accuracy. At low jet multiplicities, shape discrepancies between the measurements and the Monte Carlo predictions are observed. At high jet multiplicities, the shapes are better described but discrepancies in the normalisation are observed.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for 1.0 < $H_{\textrm{T2}}$ < 1.5 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.
Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for 1.5 < $H_{\textrm{T2}}$ < 2.0 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.
Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for $H_{\textrm{T2}}$ > 2.0 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Inclusive and differential cross-sections for the production of top quarks in association with a photon are measured with proton$-$proton collision data corresponding to an integrated luminosity of 139 fb$^{-1}$. The data were collected by the ATLAS detector at the LHC during Run 2 between 2015 and 2018 at a centre-of-mass energy of 13 TeV. The measurements are performed in a fiducial volume defined at parton level. Events with exactly one photon, one electron and one muon of opposite sign, and at least two jets, of which at least one is $b$-tagged, are selected. The fiducial cross-section is measured to be $39.6\,^{+2.7}_{-2.3}\,\textrm{fb}$. Differential cross-sections as functions of several observables are compared with state-of-the-art Monte Carlo simulations and next-to-leading-order theoretical calculations. These include cross-sections as functions of photon kinematic variables, angular variables related to the photon and the leptons, and angular separations between the two leptons in the event. All measurements are in agreement with the predictions from the Standard Model.
The measured fiducial cross-section in the electron-muon channel. The first uncertainty is the statistical uncertainty and the second one is the systematic uncertainty.
The absolute differential cross-section measured in the fiducial phase-space as a function of the photon pT in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute differential cross-section measured in the fiducial phase-space as a function of the photon $|\eta|$ in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute differential cross-section measured in the fiducial phase-space as a function of the minimum $\Delta R$ between the photon and the leptons in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute differential cross-section measured in the fiducial phase-space as a function of the $\Delta\phi$ between the two leptons in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The absolute differential cross-section measured in the fiducial phase-space as a function of the $|\Delta\eta|$ between the two leptons in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised differential cross-section measured in the fiducial phase-space as a function of the photon pT in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised differential cross-section measured in the fiducial phase-space as a function of the photon $|\eta|$ in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised differential cross-section measured in the fiducial phase-space as a function of the minimum $\Delta R$ between the photon and the leptons in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised differential cross-section measured in the fiducial phase-space as a function of the $\Delta\phi$ between the two leptons in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The normalised differential cross-section measured in the fiducial phase-space as a function of the $|\Delta\eta|$ between the two leptons in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.
The total correlation matrix of the absolute differential cross-section measured in the fiducial phase-space as a function of the photon pT in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.
The total correlation matrix of the absolute differential cross-section measured in the fiducial phase-space as a function of the photon $|\eta|$ in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.
The total correlation matrix of the absolute differential cross-section measured in the fiducial phase-space as a function of the minimum $\Delta R$ between the photon and the leptons in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.
The total correlation matrix of the absolute differential cross-section measured in the fiducial phase-space as a function of the $\Delta\phi$ between the two leptons in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.
The total correlation matrix of the absolute differential cross-section measured in the fiducial phase-space as a function of the $|\Delta\eta|$ between the two leptons in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.
The total correlation matrix of the normalised differential cross-section measured in the fiducial phase-space as a function of the photon pT in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.
The total correlation matrix of the normalised differential cross-section measured in the fiducial phase-space as a function of the photon $|\eta|$ in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.
The total correlation matrix of the normalised differential cross-section measured in the fiducial phase-space as a function of the minimum $\Delta R$ between the photon and the leptons in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.
The total correlation matrix of the normalised differential cross-section measured in the fiducial phase-space as a function of the $\Delta\phi$ between the two leptons in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.
The total correlation matrix of the normalised differential cross-section measured in the fiducial phase-space as a function of the $|\Delta\eta|$ between the two leptons in the electron-muon channel. The individual systematic uncertainties are symmetrized before deriving the correlation matrix.
The statistical correlation matrix of all the absolute differential cross-sections measured in the fiducial phase-space in the electron-muon channel.
The statistical correlation matrix of all the normalised differential cross-sections measured in the fiducial phase-space in the electron-muon channel.
Fiducial region definition.
Differential cross-sections are measured for top-quark pair production in the all-hadronic decay mode, using proton$-$proton collision events collected by the ATLAS experiment in which all six decay jets are separately resolved. Absolute and normalised single- and double-differential cross-sections are measured at particle and parton level as a function of various kinematic variables. Emphasis is placed on well-measured observables in fully reconstructed final states, as well as on the study of correlations between the top-quark pair system and additional jet radiation identified in the event. The study is performed using data from proton$-$proton collisions at $\sqrt{s}=13~\mbox{TeV}$ collected by the ATLAS detector at CERN's Large Hadron Collider in 2015 and 2016, corresponding to an integrated luminosity of $\mbox{36.1 fb}^{-1}$. The rapidities of the individual top quarks and of the top-quark pair are well modelled by several independent event generators. Significant mismodelling is observed in the transverse momenta of the leading three jet emissions, while the leading top-quark transverse momentum and top-quark pair transverse momentum are both found to be incompatible with several theoretical predictions.
The dynamics of isolated-photon plus two-jet production in $pp$ collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset corresponding to an integrated luminosity of 36.1 fb$^{-1}$. Cross sections are measured as functions of a variety of observables, including angular correlations and invariant masses of the objects in the final state, $\gamma+jet+jet$. Measurements are also performed in phase-space regions enriched in each of the two underlying physical mechanisms, namely direct and fragmentation processes. The measurements cover the range of photon (jet) transverse momenta from 150 GeV (100 GeV) to 2 TeV. The tree-level plus parton-shower predictions from SHERPA and PYTHIA as well as the next-to-leading-order QCD predictions from SHERPA are compared with the measurements. The next-to-leading-order QCD predictions describe the data adequately in shape and normalisation except for regions of phase space such as those with high values of the invariant mass or rapidity separation of the two jets, where the predictions overestimate the data.
Measured cross sections for isolated-photon plus two-jet production as functions of $E_{\mathrm{T}}^{\gamma}$ for the total phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $p_{\mathrm{T}}^{\textrm{jet}}$ for the total phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $|y^{\textrm{jet}}|$ for the total phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $\Delta y^{\gamma-\textrm{jet}}$ for the total phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $\Delta \phi^{\gamma-\textrm{jet}}$ for the total phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $\Delta y^{\textrm{jet}-\textrm{jet}}$ for the total phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $\Delta \phi^{\textrm{jet}-\textrm{jet}}$ for the total phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $m^{\textrm{jet}-\textrm{jet}}$ for the total phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $m^{\gamma-\textrm{jet}-\textrm{jet}}$ for the total phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $E_{\mathrm{T}}^{\gamma}$ for the fragmentation-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $p_{\mathrm{T}}^{\textrm{jet}}$ for the fragmentation-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $|y^{\textrm{jet}}|$ for the fragmentation-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $\Delta y^{\gamma-\textrm{jet}}$ for the fragmentation-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $\Delta \phi^{\gamma-\textrm{jet}}$ for the fragmentation-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $\Delta y^{\textrm{jet}-\textrm{jet}}$ for the fragmentation-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $\Delta \phi^{\textrm{jet}-\textrm{jet}}$ for the fragmentation-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $m^{\textrm{jet}-\textrm{jet}}$ for the fragmentation-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $m^{\gamma-\textrm{jet}-\textrm{jet}}$ for the fragmentation-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $E_{\mathrm{T}}^{\gamma}$ for the direct-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $p_{\mathrm{T}}^{\textrm{jet}}$ for the direct-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $|y^{\textrm{jet}}|$ for the direct-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $\Delta y^{\gamma-\textrm{jet}}$ for the direct-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $\Delta \phi^{\gamma-\textrm{jet}}$ for the direct-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $\Delta y^{\textrm{jet}-\textrm{jet}}$ for the direct-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $\Delta \phi^{\textrm{jet}-\textrm{jet}}$ for the direct-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $m^{\textrm{jet}-\textrm{jet}}$ for the direct-enriched phase-space. The predictions from Sherpa NLO are also included.
Measured cross sections for isolated-photon plus two-jet production as functions of $m^{\gamma-\textrm{jet}-\textrm{jet}}$ for the direct-enriched phase-space. The predictions from Sherpa NLO are also included.
This paper describes precision measurements of the transverse momentum $p_\mathrm{T}^{\ell\ell}$ ($\ell=e,\mu$) and of the angular variable $\phi^{*}_{\eta}$ distributions of Drell-Yan lepton pairs in a mass range of 66-116 GeV. The analysis uses data from 36.1 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=13$ TeV collected by the ATLAS experiment at the LHC in 2015 and 2016. Measurements in electron-pair and muon-pair final states are performed in the same fiducial volumes, corrected for detector effects, and combined. Compared to previous measurements in proton-proton collisions at $\sqrt{s}=$7 and 8 TeV, these new measurements probe perturbative QCD at a higher centre-of-mass energy with a different composition of initial states. They reach a precision of 0.2% for the normalized spectra at low values of $p_\mathrm{T}^{\ell\ell}$. The data are compared with different QCD predictions, where it is found that predictions based on resummation approaches can describe the full spectrum within uncertainties.
Selected signal candidate events in data for both decay channels as well as the expected background contributions including their total uncertainties.
Selected signal candidate events in data for both decay channels as well as the expected background contributions including their total uncertainties.
Overview of the detector efficiency correction factors, $C_{Z}$ , for the electron and muon channels and their systematic uncertainty contributions.
Overview of the detector efficiency correction factors, $C_{Z}$ , for the electron and muon channels and their systematic uncertainty contributions.
Measured inclusive cross-section in the fiducial volume in the electron and muon decay channels at Born level and their combination as well as the theory prediction at NNLO in $\alpha_{s}$ using the CT14 PDF set.
Measured inclusive cross-section in the fiducial volume in the electron and muon decay channels at Born level and their combination as well as the theory prediction at NNLO in $\alpha_{s}$ using the CT14 PDF set.
The measured combined normalized differential cross-sections, divided by the bin-width, in the fiducial volume at Born level as well as a factor $k_{dressed}$ to translate from the Born particle level to the dressed particle level.
The measured combined normalized differential cross-sections, divided by the bin-width, in the fiducial volume at Born level as well as a factor $k_{dressed}$ to translate from the Born particle level to the dressed particle level.
The measured combined normalized differential cross-sections, divided by the bin-width, in the fiducial volume at Born level as well as a factor $k_{dressed}$ to translate from the Born particle level to the dressed particle level.
The measured combined normalized differential cross-sections, divided by the bin-width, in the fiducial volume at Born level as well as a factor $k_{dressed}$ to translate from the Born particle level to the dressed particle level.
Results of the normalized differential cross-section $1/\sigma_\mathrm{fid}\times \mathrm{d}\sigma_\mathrm{fid}/\mathrm{d}p_{T}^{ll}$ measured on born level for the $Z\rightarrow\mu\mu$ decay channel. The following naming convention is used: Stat.(Data), Stat.(MC) an Eff.(Uncor.), denote the statistical uncertainties due limited data and MC as well as the uncorrelated lepton efficiency uncertainties; Scale and Res. denote the muon momentum scale and resolution uncertainties; Muon Sag. denotes the uncertainty due to the muon sagitta bias; Eff. (Cor.), Isolation, Trigger and TTVA denote the uncertainties of the data/MC scale-factors for the correlated muon reconstruction, isolation, trigger and track-to-vertex matching efficiencies; the uncertainties due to the primary vertex z-distribution and pile-up reweighting are denoted as Z-Pos and Pile-Up, while the model and background uncertainties are summarized under Model and Bkg.. The sign-information is kept to track bin-to-bin changes.
Results of the normalized differential cross-section $1/\sigma_\mathrm{fid}\times \mathrm{d}\sigma_\mathrm{fid}/\mathrm{d}p_{T}^{ll}$ measured on born level for the $Z\rightarrow\mu\mu$ decay channel. The following naming convention is used: Stat.(Data), Stat.(MC) an Eff.(Uncor.), denote the statistical uncertainties due limited data and MC as well as the uncorrelated lepton efficiency uncertainties; Scale and Res. denote the muon momentum scale and resolution uncertainties; Muon Sag. denotes the uncertainty due to the muon sagitta bias; Eff. (Cor.), Isolation, Trigger and TTVA denote the uncertainties of the data/MC scale-factors for the correlated muon reconstruction, isolation, trigger and track-to-vertex matching efficiencies; the uncertainties due to the primary vertex z-distribution and pile-up reweighting are denoted as Z-Pos and Pile-Up, while the model and background uncertainties are summarized under Model and Bkg.. The sign-information is kept to track bin-to-bin changes.
Results of the normalized differential cross-section $1/\sigma_\mathrm{fid}\times \mathrm{d}\sigma_\mathrm{fid}/\mathrm{d}\phi_{\eta}^{*}$ measured on born level for the $Z\rightarrow\mu\mu$ decay channel. The following naming convention is used: Stat.(Data), Stat.(MC) an Eff.(Uncor.), denote the statistical uncertainties due limited data and MC as well as the uncorrelated lepton efficiency uncertainties; Scale and Res. denote the muon momentum scale and resolution uncertainties; Muon Sag. denotes the uncertainty due to the muon sagitta bias; Eff. (Cor.), Isolation, Trigger and TTVA denote the uncertainties of the data/MC scale-factors for the correlated muon reconstruction, isolation, trigger and track-to-vertex matching efficiencies; the uncertainties due to the primary vertex z-distribution and pile-up reweighting are denoted as Z-Pos and Pile-Up, while the model and background uncertainties are summarized under Model and Bkg.. The sign-information is kept to track bin-to-bin changes.
Results of the normalized differential cross-section $1/\sigma_\mathrm{fid}\times \mathrm{d}\sigma_\mathrm{fid}/\mathrm{d}\phi_{\eta}^{*}$ measured on born level for the $Z\rightarrow\mu\mu$ decay channel. The following naming convention is used: Stat.(Data), Stat.(MC) an Eff.(Uncor.), denote the statistical uncertainties due limited data and MC as well as the uncorrelated lepton efficiency uncertainties; Scale and Res. denote the muon momentum scale and resolution uncertainties; Muon Sag. denotes the uncertainty due to the muon sagitta bias; Eff. (Cor.), Isolation, Trigger and TTVA denote the uncertainties of the data/MC scale-factors for the correlated muon reconstruction, isolation, trigger and track-to-vertex matching efficiencies; the uncertainties due to the primary vertex z-distribution and pile-up reweighting are denoted as Z-Pos and Pile-Up, while the model and background uncertainties are summarized under Model and Bkg.. The sign-information is kept to track bin-to-bin changes.
Results of the normalized differential cross-section $1/\sigma_\mathrm{fid}\times \mathrm{d}\sigma_\mathrm{fid}/\mathrm{d}p_{T}^{ll}$ measured on born level for the $Z\rightarrow ee$ decay channel. The following naming convention is used: Stat.(Data), Stat.(MC) and Eff.(Uncor.), denote the statistical uncertainties due limited data and MC as well as the uncorrelated lepton efficiency uncertainties; Scale and Res. for the electron momentum scale and resolution uncertainties; Elec. (Reco), Elec. (ID), Isolation, Trigger and Charge-ID denote the correlated uncertainties of the data/MC scale-factors for the electron reconstruction, identification, isolation, trigger and charge-identification efficiencies; The uncertainties due to the primary vertex z-distribution and pile-up reweighting are denoted as Z-Pos and Pile-Up, while the model and background uncertainties are summarized under Model and Bkg. The sign-information is kept to track bin-to-bin changes.
Results of the normalized differential cross-section $1/\sigma_\mathrm{fid}\times \mathrm{d}\sigma_\mathrm{fid}/\mathrm{d}p_{T}^{ll}$ measured on born level for the $Z\rightarrow ee$ decay channel. The following naming convention is used: Stat.(Data), Stat.(MC) and Eff.(Uncor.), denote the statistical uncertainties due limited data and MC as well as the uncorrelated lepton efficiency uncertainties; Scale and Res. for the electron momentum scale and resolution uncertainties; Elec. (Reco), Elec. (ID), Isolation, Trigger and Charge-ID denote the correlated uncertainties of the data/MC scale-factors for the electron reconstruction, identification, isolation, trigger and charge-identification efficiencies; The uncertainties due to the primary vertex z-distribution and pile-up reweighting are denoted as Z-Pos and Pile-Up, while the model and background uncertainties are summarized under Model and Bkg. The sign-information is kept to track bin-to-bin changes.
Results of the normalized differential cross-section $1/\sigma_\mathrm{fid} \times \mathrm{d}\sigma_\mathrm{fid}/\mathrm{d}\phi_{\eta}^{*}$ measured on born level for the $Z\rightarrow ee$ decay channel. The following naming convention is used: Stat.(Data), Stat.(MC) and Eff.(Uncor.), denote the statistical uncertainties due limited data and MC as well as the uncorrelated lepton efficiency uncertainties; Scale and Res. for the electron momentum scale and resolution uncertainties; Elec. (Reco), Elec. (ID), Isolation, Trigger and Charge-ID denote the correlated uncertainties of the data/MC scale-factors for the electron reconstruction, identification, isolation, trigger and charge-identification efficiencies; The uncertainties due to the primary vertex z-distribution and pile-up reweighting are denoted as Z-Pos and Pile-Up, while the model and background uncertainties are summarized under Model and Bkg. The sign-information is kept to track bin-to-bin changes.
Results of the normalized differential cross-section $1/\sigma_\mathrm{fid} \times \mathrm{d}\sigma_\mathrm{fid}/\mathrm{d}\phi_{\eta}^{*}$ measured on born level for the $Z\rightarrow ee$ decay channel. The following naming convention is used: Stat.(Data), Stat.(MC) and Eff.(Uncor.), denote the statistical uncertainties due limited data and MC as well as the uncorrelated lepton efficiency uncertainties; Scale and Res. for the electron momentum scale and resolution uncertainties; Elec. (Reco), Elec. (ID), Isolation, Trigger and Charge-ID denote the correlated uncertainties of the data/MC scale-factors for the electron reconstruction, identification, isolation, trigger and charge-identification efficiencies; The uncertainties due to the primary vertex z-distribution and pile-up reweighting are denoted as Z-Pos and Pile-Up, while the model and background uncertainties are summarized under Model and Bkg. The sign-information is kept to track bin-to-bin changes.
Results of the normalized differential cross-section $1/\sigma_\mathrm{fid} \times \mathrm{d}\sigma_\mathrm{fid}/\mathrm{d}p_{T}^{ll}$ measured on bare level for the $Z\rightarrow\mu\mu$ decay channel. The following naming convention is used: Stat.(Data), Stat.(MC) an Eff.(Uncor.), denote the statistical uncertainties due limited data and MC as well as the uncorrelated lepton efficiency uncertainties; Scale and Res. denote the muon momentum scale and resolution uncertainties; Muon Sag. denotes the uncertainty due to the muon sagitta bias; Eff. (Cor.), Isolation, Trigger and TTVA denote the uncertainties of the data/MC scale-factors for the correlated muon reconstruction, isolation, trigger and track-to-vertex matching efficiencies; the uncertainties due to the primary vertex z-distribution and pile-up reweighting are denoted as Z-Pos and Pile-Up, while the model and background uncertainties are summarized under Model and Bkg.. The sign-information is kept to track bin-to-bin changes.
Results of the normalized differential cross-section $1/\sigma_\mathrm{fid} \times \mathrm{d}\sigma_\mathrm{fid}/\mathrm{d}p_{T}^{ll}$ measured on bare level for the $Z\rightarrow\mu\mu$ decay channel. The following naming convention is used: Stat.(Data), Stat.(MC) an Eff.(Uncor.), denote the statistical uncertainties due limited data and MC as well as the uncorrelated lepton efficiency uncertainties; Scale and Res. denote the muon momentum scale and resolution uncertainties; Muon Sag. denotes the uncertainty due to the muon sagitta bias; Eff. (Cor.), Isolation, Trigger and TTVA denote the uncertainties of the data/MC scale-factors for the correlated muon reconstruction, isolation, trigger and track-to-vertex matching efficiencies; the uncertainties due to the primary vertex z-distribution and pile-up reweighting are denoted as Z-Pos and Pile-Up, while the model and background uncertainties are summarized under Model and Bkg.. The sign-information is kept to track bin-to-bin changes.
Results of the normalized differential cross-section $1/\sigma_\mathrm{fid} \times \mathrm{d}\sigma_\mathrm{fid}/\mathrm{d}\phi_{\eta}^{*}$ measured on bare level for the $Z\rightarrow\mu\mu$ decay channel. The following naming convention is used: Stat.(Data), Stat.(MC) an Eff.(Uncor.), denote the statistical uncertainties due limited data and MC as well as the uncorrelated lepton efficiency uncertainties; Scale and Res. denote the muon momentum scale and resolution uncertainties; Muon Sag. denotes the uncertainty due to the muon sagitta bias; Eff. (Cor.), Isolation, Trigger and TTVA denote the uncertainties of the data/MC scale-factors for the correlated muon reconstruction, isolation, trigger and track-to-vertex matching efficiencies; the uncertainties due to the primary vertex z-distribution and pile-up reweighting are denoted as Z-Pos and Pile-Up, while the model and background uncertainties are summarized under Model and Bkg.. The sign-information is kept to track bin-to-bin changes.
Results of the normalized differential cross-section $1/\sigma_\mathrm{fid} \times \mathrm{d}\sigma_\mathrm{fid}/\mathrm{d}\phi_{\eta}^{*}$ measured on bare level for the $Z\rightarrow\mu\mu$ decay channel. The following naming convention is used: Stat.(Data), Stat.(MC) an Eff.(Uncor.), denote the statistical uncertainties due limited data and MC as well as the uncorrelated lepton efficiency uncertainties; Scale and Res. denote the muon momentum scale and resolution uncertainties; Muon Sag. denotes the uncertainty due to the muon sagitta bias; Eff. (Cor.), Isolation, Trigger and TTVA denote the uncertainties of the data/MC scale-factors for the correlated muon reconstruction, isolation, trigger and track-to-vertex matching efficiencies; the uncertainties due to the primary vertex z-distribution and pile-up reweighting are denoted as Z-Pos and Pile-Up, while the model and background uncertainties are summarized under Model and Bkg.. The sign-information is kept to track bin-to-bin changes.
Measured combined normalized differential cross-section in the fiducial volume at Born level as well as a factor $k_{dressed}$ to translate from the Born particle level to the dressed particle.
Measured combined normalized differential cross-section in the fiducial volume at Born level as well as a factor $k_{dressed}$ to translate from the Born particle level to the dressed particle.
Measured combined normalized differential cross-section in the fiducial volume at Born level as well as a factor $k_{dressed}$ to translate from the Born particle level to the dressed particle.
Measured combined normalized differential cross-section in the fiducial volume at Born level as well as a factor $k_{dressed}$ to translate from the Born particle level to the dressed particle.
The distribution of events passing the selection requirements in the electron channel as a function of dilepton invariant mass $m_{ll}$ , the latter with one entry for each lepton per event. The MC signal sample is simulated using Powheg+Pythia8. The predictions of the MC signal sample together with the MC background samples are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the electron channel as a function of dilepton invariant mass $m_{ll}$ , the latter with one entry for each lepton per event. The MC signal sample is simulated using Powheg+Pythia8. The predictions of the MC signal sample together with the MC background samples are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the muon channel as a function of dilepton invariant mass $m_{ll}$, the latter with one entry for each lepton per event. The MC signal sample is simulated using Powheg+Pythia8. The predictions of the MC signal sample together with the MC background samples are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the muon channel as a function of dilepton invariant mass $m_{ll}$, the latter with one entry for each lepton per event. The MC signal sample is simulated using Powheg+Pythia8. The predictions of the MC signal sample together with the MC background samples are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the electron channel as a function of lepton pseudorapidity $\eta$, the latter with one entry for each lepton per event. The MC signal sample is simulated using Powheg+Pythia8. The predictions of the MC signal sample together with the MC background samples are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the electron channel as a function of lepton pseudorapidity $\eta$, the latter with one entry for each lepton per event. The MC signal sample is simulated using Powheg+Pythia8. The predictions of the MC signal sample together with the MC background samples are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the muon channel as a function of lepton pseudorapidity $\eta$, the latter with one entry for each lepton per event. The MC signal sample is simulated using Powheg+Pythia8. The predictions of the MC signal sample together with the MC background samples are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the muon channel as a function of lepton pseudorapidity $\eta$, the latter with one entry for each lepton per event. The MC signal sample is simulated using Powheg+Pythia8. The predictions of the MC signal sample together with the MC background samples are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the electron channel as a function of dilepton transverse momentum. The MC signal sample is simulated using Powheg+Pythia8. The predictions are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the electron channel as a function of dilepton transverse momentum. The MC signal sample is simulated using Powheg+Pythia8. The predictions are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the muon channel as a function of dilepton transverse momentum. The MC signal sample is simulated using Powheg+Pythia8. The predictions are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the muon channel as a function of dilepton transverse momentum. The MC signal sample is simulated using Powheg+Pythia8. The predictions are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the electron channel as a function of $\phi_{\eta}^{*}$. The MC signal sample is simulated using Powheg+Pythia8. The predictions are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the electron channel as a function of $\phi_{\eta}^{*}$. The MC signal sample is simulated using Powheg+Pythia8. The predictions are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the muon channel as a function of $\phi_{\eta}^{*}$. The MC signal sample is simulated using Powheg+Pythia8. The predictions are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The distribution of events passing the selection requirements in the muon channel as a function of $\phi_{\eta}^{*}$. The MC signal sample is simulated using Powheg+Pythia8. The predictions are normalized to the integral of the data and the total experimental uncertainty of the predicted values is shown as a grey band in the ratio of the prediction to data.
The measured normalized cross section as a function of $p_{ll}$ for the electron and muon channels and the combined result as well as their ratio together with the total uncertainties, shown as a blue band. The pull distribution between the electron and muon channels, defined as the difference between the two channels divided by the combined uncorrelated uncertainty, is also shown. The $p_{ll}$ distribution is split into linear and logarithmic scales at 30 GeV.
The measured normalized cross section as a function of $p_{ll}$ for the electron and muon channels and the combined result as well as their ratio together with the total uncertainties, shown as a blue band. The pull distribution between the electron and muon channels, defined as the difference between the two channels divided by the combined uncorrelated uncertainty, is also shown. The $p_{ll}$ distribution is split into linear and logarithmic scales at 30 GeV.
The measured normalized cross section as a function of $\phi_{\eta}^{*}$ for the electron and muon channels and the combined result as well as their ratio together with the total uncertainties, shown as a blue band. The pull distribution between the electron and muon channels, defined as the difference between the two channels divided by the combined uncorrelated uncertainty, is also shown.
The measured normalized cross section as a function of $\phi_{\eta}^{*}$ for the electron and muon channels and the combined result as well as their ratio together with the total uncertainties, shown as a blue band. The pull distribution between the electron and muon channels, defined as the difference between the two channels divided by the combined uncorrelated uncertainty, is also shown.
Comparison of the normalized $p_{ll}$ distributions predicted by different computations: Pythia8 with the AZ tune, Powheg+Pythia8 with the AZNLO tune, Sherpa v2.2.1 and RadISH with the Born level combined measurement. The uncertainties of the measurement are shown as vertical bars and uncertainties of the Sherpa and RadISH predictions are indicated by the coloured bands.
Comparison of the normalized $p_{ll}$ distributions predicted by different computations: Pythia8 with the AZ tune, Powheg+Pythia8 with the AZNLO tune, Sherpa v2.2.1 and RadISH with the Born level combined measurement. The uncertainties of the measurement are shown as vertical bars and uncertainties of the Sherpa and RadISH predictions are indicated by the coloured bands.
Comparison of the normalized $\phi_{\eta}^{*}$ distributions predicted by different computations: Pythia8 with the AZ tune, Powheg+Pythia8 with the AZNLO tune, Sherpa v2.2.1 and RadISH with the Born level combined measurement. The uncertainties of the measurement are shown as vertical bars and uncertainties of the Sherpa and RadISH predictions are indicated by the coloured bands.
Comparison of the normalized $\phi_{\eta}^{*}$ distributions predicted by different computations: Pythia8 with the AZ tune, Powheg+Pythia8 with the AZNLO tune, Sherpa v2.2.1 and RadISH with the Born level combined measurement. The uncertainties of the measurement are shown as vertical bars and uncertainties of the Sherpa and RadISH predictions are indicated by the coloured bands.
Comparison of the normalized $p_{ll}$ distribution in the range $p_{ll}$ > 10 GeV. The Born level combined measurement is compared with predictions by Sherpa v2.2.1, fixed-order NNLOjet and NNLOjet supplied with NLO electroweak corrections. The uncertainties in the measurement are shown as vertical bars and the uncertainties in the predictions are indicated by the coloured bands.
Comparison of the normalized $p_{ll}$ distribution in the range $p_{ll}$ > 10 GeV. The Born level combined measurement is compared with predictions by Sherpa v2.2.1, fixed-order NNLOjet and NNLOjet supplied with NLO electroweak corrections. The uncertainties in the measurement are shown as vertical bars and the uncertainties in the predictions are indicated by the coloured bands.
Single- and double-differential cross-section measurements are presented for the production of top-quark pairs, in the lepton + jets channel at particle and parton level. Two topologies, resolved and boosted, are considered and the results are presented as a function of several kinematic variables characterising the top and $t\bar{t}$ system and jet multiplicities. The study was performed using data from $pp$ collisions at centre-of-mass energy of 13 TeV collected in 2015 and 2016 by the ATLAS detector at the CERN Large Hadron Collider (LHC), corresponding to an integrated luminosity of $36~\mathrm{fb}^{-1}$. Due to the large $t\bar{t}$ cross-section at the LHC, such measurements allow a detailed study of the properties of top-quark production and decay, enabling precision tests of several Monte Carlo generators and fixed-order Standard Model predictions. Overall, there is good agreement between the theoretical predictions and the data.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $m^{t\bar{t}}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute differential cross-section as a function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|y_{boost}^{t\bar{t}}|$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 400.0 GeV < $m^{t\bar{t}}$ < 550.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 200.0 GeV < $m^{t\bar{t}}$ < 400.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at particle level in the resolved topology in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 550.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 200.0 GeV < $p_{T}^{t,had}$ < 300.0 GeV and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 60.0 GeV < $p_{T}^{t,had}$ < 120.0 GeV and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $p_{T}^{t,had}$ in 0.0 GeV < $p_{T}^{t,had}$ < 60.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Absolute double-differential cross-section as function of $|p_{out}^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 and the Relative double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 6.5 < $N^{jets}$ < 7.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 3.5 < $N^{jets}$ < 4.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 and the Absolute double-differential cross-section as function of $\Delta\phi(t,\bar{t})$ vs $N^{jets}$ in 4.5 < $N^{jets}$ < 5.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $H_{T}^{t\bar{t}}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $|y^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $|y^{t,had}|$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 6.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 and the Relative double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t,had}|$ vs $N^{jets}$ in $N^{jets}$ = 6.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 and the Absolute double-differential cross-section as function of $|y^{t\bar{t}}|$ vs $N^{jets}$ in $N^{jets}$ $\geq$ 7.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 4.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 and the Relative double-differential cross-section as function of $\chi_{tt}$ vs $N^{jets}$ in $N^{jets}$ = 5.0 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $\chi_{tt}$ vs $N^{jets}$ at particle level in the resolved topology in $N^{jets}$ = 4.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.4 < $|y^{t,had}|$ < 2.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.8 < $|y^{t\bar{t}}|$ < 1.2 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.0 < $|y^{t\bar{t}}|$ < 0.4 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 1.2 < $|y^{t\bar{t}}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 1.2 < $|y^{t\bar{t}}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.0 < $|y^{t\bar{t}}|$ < 0.4 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.4 < $|y^{t\bar{t}}|$ < 0.8 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 0.8 < $|y^{t\bar{t}}|$ < 1.2 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the resolved topology in 1.2 < $|y^{t\bar{t}}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.4 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.4 < $|y^{t\bar{t}}|$ < 0.8 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.2 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.8 < $|y^{t\bar{t}}|$ < 1.2 at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the resolved topology in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 30.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 30.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 190.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 190.0 GeV at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,had}|$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $N^{extra jets}$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|p_{out}^{t,had}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|\Delta\phi(t,\bar{t})|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $N^{extra jets}$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at particle level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the resolved topology.
Relative differential cross-section as a function of $p_{T}^{t}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $p_{T}^{t}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|y^{t}|$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|y^{t}|$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $m^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $m^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|y^{t\bar{t}}|$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|y^{t\bar{t}}|$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $\chi_{tt}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $\chi_{tt}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $\chi_{tt}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $\chi_{tt}$ at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $|y^{t}|$ at parton level in the resolved topology in 0.0 < $|y^{t}|$ < 0.75 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $|y^{t}|$ at parton level in the resolved topology in 0.75 < $|y^{t}|$ < 1.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $|y^{t}|$ at parton level in the resolved topology in 1.5 < $|y^{t}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $|y^{t}|$ at parton level in the resolved topology in 0.0 < $|y^{t}|$ < 0.75 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $|y^{t}|$ at parton level in the resolved topology in 0.75 < $|y^{t}|$ < 1.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $|y^{t}|$ at parton level in the resolved topology in 1.5 < $|y^{t}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.0 < $|y^{t}|$ < 0.75 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 0.75 < $|y^{t}|$ < 1.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $|y^{t}|$ in 1.5 < $|y^{t}|$ < 2.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ at parton level in the resolved topology in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 80.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 80.0 GeV < $p_{T}^{t\bar{t}}$ < 180.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 180.0 GeV < $p_{T}^{t\bar{t}}$ < 330.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $p_{T}^{t\bar{t}}$ in 330.0 GeV < $p_{T}^{t\bar{t}}$ < 800.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 GeV < $|y^{t\bar{t}}|$ < 1.1 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 GeV < $|y^{t\bar{t}}|$ < 0.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 GeV < $|y^{t\bar{t}}|$ < 1.7 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 GeV < $|y^{t\bar{t}}|$ < 2.5 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ at parton level in the resolved topology in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 325.0 GeV < $m^{t\bar{t}}$ < 500.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 500.0 GeV < $m^{t\bar{t}}$ < 700.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 700.0 GeV < $m^{t\bar{t}}$ < 1000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $m^{t\bar{t}}$ in 1000.0 GeV < $m^{t\bar{t}}$ < 2000.0 GeV at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.0 < $|y^{t\bar{t}}|$ < 0.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.5 < $|y^{t\bar{t}}|$ < 1.1 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.1 < $|y^{t\bar{t}}|$ < 1.7 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.7 < $|y^{t\bar{t}}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.0 < $|y^{t\bar{t}}|$ < 0.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 0.5 < $|y^{t\bar{t}}|$ < 1.1 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.1 < $|y^{t\bar{t}}|$ < 1.7 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at parton level in the resolved topology in 1.7 < $|y^{t\bar{t}}|$ < 2.5 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.5 < $|y^{t\bar{t}}|$ < 1.1 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.1 < $|y^{t\bar{t}}|$ < 1.7 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.7 < $|y^{t\bar{t}}|$ < 2.5 at parton level in the resolved topology, accounting for the statistical and systematic uncertainties.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t}|$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t}|$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $p_{T}^{t}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $|y^{t}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $|y_{boost}^{t\bar{t}}|$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at parton level in the resolved topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi_{tt}$ and the absolute differential cross-section as function of $\chi_{tt}$ at parton level in the resolved topology.
Absolute differential cross-section as a function of $p_{T}^{t}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute differential cross-section as a function of $y^{t}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute differential cross-section as a function of $m^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute differential cross-section as a function of $p_{T}^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute differential cross-section as a function of $y^{t\bar{t}}$ at parton level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative differential cross-section as a function of $p_{T}^{t,had}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $p_{T}^{t,had}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|y^{t,had}|$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|y^{t,had}|$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $p_{T}^{t,1}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $p_{T}^{t,1}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $p_{T}^{t,2}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $p_{T}^{t,2}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|y^{t\bar{t}}|$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|y^{t\bar{t}}|$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $m^{t\bar{t}}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $m^{t\bar{t}}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $\chi^{t\bar{t}}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $\chi^{t\bar{t}}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $|p_{out}^{t,lep}|$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $H_{T}^{t\bar{t}}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $H_{T}^{t\bar{t}}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $H_{T}^{t\bar{t}}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $N^{extra jets}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $N^{extra jets}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $N^{extra jets}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $N^{extra jets}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative differential cross-section as a function of $N^{subjets}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $N^{subjets}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute differential cross-section as a function of $N^{subjets}$ at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of $N^{subjets}$ at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Total cross-section at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 0.0 < $|y^{t\bar{t}}|$ < 1.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 1.0 < $|y^{t\bar{t}}|$ < 2.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 0.0 < $|y^{t\bar{t}}|$ < 1.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 1.0 < $|y^{t\bar{t}}|$ < 2.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t\bar{t}}|$ in 1.0 < $|y^{t\bar{t}}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the boosted topology in 0.0 < $|y^{t,had}|$ < 1.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the boosted topology in 1.0 < $|y^{t,had}|$ < 2.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the boosted topology in 0.0 < $|y^{t,had}|$ < 1.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ at particle level in the boosted topology in 1.0 < $|y^{t,had}|$ < 2.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 1.0 < $|y^{t,had}|$ < 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $|y^{t,had}|$ in 0.0 < $|y^{t,had}|$ < 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the boosted topology in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the boosted topology in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ at particle level in the boosted topology in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 490.0 GeV < $m^{t\bar{t}}$ < 1160.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $m^{t\bar{t}}$ in 1160.0 GeV < $m^{t\bar{t}}$ < 3000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ at particle level in the boosted topology in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ at particle level in the boosted topology in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ at particle level in the boosted topology in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ at particle level in the boosted topology in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 350.0 GeV < $H_{T}^{t\bar{t}}$ < 780.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $H_{T}^{t\bar{t}}$ in 780.0 GeV < $H_{T}^{t\bar{t}}$ < 2500.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ at particle level in the boosted topology in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 0.0 GeV < $p_{T}^{t\bar{t}}$ < 40.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 40.0 GeV < $p_{T}^{t\bar{t}}$ < 150.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $p_{T}^{t\bar{t}}$ in 150.0 GeV < $p_{T}^{t\bar{t}}$ < 1000.0 GeV at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 0.0 < $|y^{t\bar{t}}|$ < 0.65 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 0.65 < $|y^{t\bar{t}}|$ < 1.3 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 1.3 < $|y^{t\bar{t}}|$ < 2.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 0.0 < $|y^{t\bar{t}}|$ < 0.65 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 0.65 < $|y^{t\bar{t}}|$ < 1.3 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ at particle level in the boosted topology in 1.3 < $|y^{t\bar{t}}|$ < 2.0 . Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.0 < $|y^{t\bar{t}}|$ < 0.65 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 0.65 < $|y^{t\bar{t}}|$ < 1.3 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $|y^{t\bar{t}}|$ in 1.3 < $|y^{t\bar{t}}|$ < 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 0.5. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ $\geq$ 3.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Relative double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 0.5. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 2.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t,had}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ $\geq$ 3.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 and the Absolute double-differential cross-section as function of $p_{T}^{t,had}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 3.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 0.5. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ $\geq$ 2.5. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 and the Relative double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 0.5. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ $\geq$ 2.5. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 and the Absolute double-differential cross-section as function of $p_{T}^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.5 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 0.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 1.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Relative double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ $\geq$ 2.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Relative double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ = 1.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Absolute double-differential cross-section as a function of $m^{t\bar{t}}$ vs $N^{extra jets}$ at particle level in the boosted topology in $N^{extra jets}$ $\geq$ 2.0. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 0.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ = 1.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Covariance matrix between the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 and the Absolute double-differential cross-section as function of $m^{t\bar{t}}$ vs $N^{extra jets}$ in $N^{extra jets}$ $\geq$ 2.0 at particle level in the boosted topology, accounting for the statistical and systematic uncertainties.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,had}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t,had}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t,had}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,1}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t,2}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|y^{t\bar{t}}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $m^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $m^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $\chi^{t\bar{t}}$ and the absolute differential cross-section as function of $\chi^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $p_{T}^{t,had}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $|y^{t,had}|$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $p_{T}^{t,1}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $p_{T}^{t,2}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the boosted topology.
Statistical correlation matrix between the absolute differential cross-section as function of $|p_{out}^{t,lep}|$ and the absolute differential cross-section as function of $|y^{t\bar{t}}|$ at particle level in the boosted topology.
Covariance matrix of the Relative differential cross-section as function of $m^{t\bar{t}}$ at parton level in the boosted topology, accounting for the statistical and systematic uncertainties.
The differential cross section for isolated-photon production in $pp$ collisions is measured at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC using an integrated luminosity of 36.1 fb$^{-1}$. The differential cross section is presented as a function of the photon transverse energy in different regions of photon pseudorapidity. The differential cross section as a function of the absolute value of the photon pseudorapidity is also presented in different regions of photon transverse energy. Next-to-leading-order QCD calculations from JETPHOX and SHERPA as well as next-to-next-to-leading-order QCD calculations from NNLOJET are compared with the measurement, using several parameterisations of the proton parton distribution functions. The predictions provide a good description of the data within the experimental and theoretical uncertainties.
Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$.
Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<1.37$.
Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$.
Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.37$.
Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$.
Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<1.37$.
Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$.
Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.37$.
A measurement of fiducial and differential cross-sections for $W^+W^-$ production in proton-proton collisions at $\sqrt{s}=$13 TeV with the ATLAS experiment at the Large Hadron Collider using data corresponding to an integrated luminosity of $36.1$ fb$^{-1}$ is presented. Events with one electron and one muon are selected, corresponding to the decay of the diboson system as $WW\rightarrow e^{\pm}\nu\mu^{\mp}\nu$. To suppress top-quark background, events containing jets with a transverse momentum exceeding 35 GeV are not included in the measurement phase space. The fiducial cross-section, six differential distributions and the cross-section as a function of the jet-veto transverse momentum threshold are measured and compared with several theoretical predictions. Constraints on anomalous electroweak gauge boson self-interactions are also presented in the framework of a dimension-six effective field theory.
Measured fiducial cross-section as a function of the jet-veto $p_{T}$ threshold. The value at the jet-veto $p_{T}$ threshold of 35GeV corresponds to the nominal fiducial cross section measured in this publication.
Statistical correlation between bins in data for the measured fiducial cross-section as a function of the jet-veto $p_{T}$ threshold. The value at the jet-veto $p_{T}$ threshold of 35GeV corresponds to the nominal fiducial cross section measured in this publication.
Total correlation between bins in data for the measured fiducial cross-section as a function of the jet-veto $p_{T}$ threshold. The value at the jet-veto $p_{T}$ threshold of 35GeV corresponds to the nominal fiducial cross section measured in this publication.
Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.
Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.
Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.
Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.
Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.
Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.
Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.
Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.
Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.
Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.
Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.
Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.
Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.
Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.
Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.
Measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.
Statistical correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.
Total correlation between bins in data for the measured fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.
Measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.
Statistical correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.
Total correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_\text{T}^{\text{lead }\ell}$.
Measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.
Statistical correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.
Total correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $m_{e\mu}$.
Measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.
Statistical correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.
Total correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $p_{T}^{e\mu}$.
Measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.
Statistical correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.
Total correlation between bins in data for the measured normalized fiducial cross-section of $WW\rightarrow e\mu$ production for the observable $|y_{e\mu}|$.
Measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.
Statistical correlation between bins in data for the measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.
Total correlation between bins in data for the measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $\Delta\phi_{e\mu}$.
Measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.
Statistical correlation between bins in data for the measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.
Total correlation between bins in data for the measured normalized fiducial cross section of $WW\rightarrow e\mu$ production for the observable $|cos(\theta^*)|$.
List of experimentally considered systematic uncertainties for the WW cross section measurement.
Extrapolated unfolded fiducial cross-section of $WW\rightarrow e\mu$ production as a function of $p_\text{T}^{\text{lead }\ell}$.
Extrapolated unfolded fiducial cross-section of $WW\rightarrow e\mu$ production as a function of $m_{e\mu}$.
Extrapolated unfolded fiducial cross-section of $WW\rightarrow e\mu$ production as a function of $p_{T}^{e\mu}$.
The inclusive production rates of isolated, prompt photons in $p$+Pb collisions at $\sqrt{s_\mathrm{NN}} = 8.16$ TeV are studied with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{-1}$ recorded in 2016. The cross-section and nuclear modification factor $R_{p\mathrm{Pb}}$ are measured as a function of photon transverse energy from 20 GeV to 550 GeV and in three nucleon-nucleon centre-of-mass pseudorapidity regions, (-2.83,-2.02), (-1.84,0.91), and (1.09,1.90). The cross-section and $R_{p\mathrm{Pb}}$ values are compared with the results of a next-to-leading-order perturbative QCD calculation, with and without nuclear parton distribution function modifications, and with expectations based on a model of the energy loss of partons prior to the hard scattering. The data disfavour a large amount of energy loss and provide new constraints on the parton densities in nuclei.
The measured cross sections for prompt, isolated photons with rapidity in (1.09,1.90).
The measured cross sections for prompt, isolated photons with rapidity in (−1.84,0.91).
The measured cross sections for prompt, isolated photons with rapidity in (−2.83,−2.02).
The nuclear modification factor R_pPb for prompt, isolated photons with rapidity in (1.09,1.90).
The nuclear modification factor R_pPb for prompt, isolated photons with rapidity in (−1.84,0.91).
The nuclear modification factor R_pPb for prompt, isolated photons with rapidity in (−2.83,−2.02).
The ratio of R_{pPb} from rapidity (1.09,1.90) to that of rapidity (−2.83,−2.02).
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